11,147 research outputs found

    Producing graphite with desired properties

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    Isotropic or anisotropic graphite is synthesized with precise control of particle size, distribution, and shape. The isotropic graphites are nearly perfectly isotropic, with thermal expansion coefficients two or three times those of ordinary graphites. The anisotropic graphites approach the anisotropy of pyrolytic graphite

    Using the local gyrokinetic code, GS2, to investigate global ITG modes in tokamaks. (I) s-α{\alpha} model with profile and flow shear effects

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    This paper combines results from a local gyrokinetic code with analytical theory to reconstruct the global eigenmode structure of the linearly unstable ion-temperature-gradient (ITG) mode with adiabatic electrons. The simulations presented here employ the s-α{\alpha} tokamak equilibrium model. Local gyrokinetic calculations, using GS2 have been performed over a range of radial surfaces, x, and for ballooning phase angle, p, in the range -π≤p≤π{\pi} {\leq} p {\leq\pi}, to map out the complex local mode frequency, Ω0(x,p)=ω0(x,p)+iγ0(x,p){\Omega_0(x, p) = \omega_0(x, p) + i\gamma_0(x, p)}. Assuming a quadratic radial profile for the drive, namely ηi=Ln/LT{\eta_i = L_n/L_T}, (holding constant all other equilibrium profiles such as safety factor, magnetic shear etc.), Ω0(x,p){\Omega_0(x, p)} has a stationary point. The reconstructed global mode then sits on the outboard mid plane of the tokamak plasma, and is known as a conventional or isolated mode, with global growth rate, γ{\gamma} ~ Max[γ0(x,p){\gamma_0(x, p)}], where γ0(x,p){\gamma_0(x, p)} is the local growth rate. Taking the radial variation in other equilibrium profiles (e.g safety factor q(x)) into account, removes the stationary point in Ω0(x,p){\Omega_0(x, p)} and results in a mode that peaks slightly away from the outboard mid-plane with a reduced global growth rate. Finally, the influence of flow shear has also been investigated through a Doppler shift, ω0→ω0+nΩ′x{\omega_0 \rightarrow \omega_0 + n\Omega^{\prime}x}, where n is the toroidal mode number and Ω′{\Omega^{\prime}} incorporates the effect of flow shear. The equilibrium profile variation introduces an asymmetry to the growth rate spectrum with respect to the sign of Ω′{\Omega^{\prime}}, consistent with recent global gyrokinetic calculations.Comment: 10 pages, 8 figures and 1 tabl

    Multi-camera Realtime 3D Tracking of Multiple Flying Animals

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    Automated tracking of animal movement allows analyses that would not otherwise be possible by providing great quantities of data. The additional capability of tracking in realtime - with minimal latency - opens up the experimental possibility of manipulating sensory feedback, thus allowing detailed explorations of the neural basis for control of behavior. Here we describe a new system capable of tracking the position and body orientation of animals such as flies and birds. The system operates with less than 40 msec latency and can track multiple animals simultaneously. To achieve these results, a multi target tracking algorithm was developed based on the Extended Kalman Filter and the Nearest Neighbor Standard Filter data association algorithm. In one implementation, an eleven camera system is capable of tracking three flies simultaneously at 60 frames per second using a gigabit network of nine standard Intel Pentium 4 and Core 2 Duo computers. This manuscript presents the rationale and details of the algorithms employed and shows three implementations of the system. An experiment was performed using the tracking system to measure the effect of visual contrast on the flight speed of Drosophila melanogaster. At low contrasts, speed is more variable and faster on average than at high contrasts. Thus, the system is already a useful tool to study the neurobiology and behavior of freely flying animals. If combined with other techniques, such as `virtual reality'-type computer graphics or genetic manipulation, the tracking system would offer a powerful new way to investigate the biology of flying animals.Comment: pdfTeX using libpoppler 3.141592-1.40.3-2.2 (Web2C 7.5.6), 18 pages with 9 figure

    Structure of Micro-instabilities in Tokamak Plasmas: Stiff Transport or Plasma Eruptions?

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    Solutions to a model 2D eigenmode equation describing micro-instabilities in tokamak plasmas are presented that demonstrate a sensitivity of the mode structure and stability to plasma profiles. In narrow regions of parameter space, with special plasma profiles, a maximally unstable mode is found that balloons on the outboard side of the tokamak. This corresponds to the conventional picture of a ballooning mode. However, for most profiles this mode cannot exist and instead a more stable mode is found that balloons closer to the top or bottom of the plasma. Good quantitative agreement with a 1D ballooning analysis is found provided the constraints associated with higher order profile effects, often neglected, are taken into account. A sudden transition from this general mode to the more unstable ballooning mode can occur for a critical flow shear, providing a candidate model for why some experiments observe small plasma eruptions (Edge Localised Modes, or ELMs) in place of large Type I ELMs.Comment: 11 pages, 3 figure

    Kinetic instabilities that limit {\beta} in the edge of a tokamak plasma: a picture of an H-mode pedestal

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    Plasma equilibria reconstructed from the Mega-Amp Spherical Tokamak (MAST) have sufficient resolution to capture plasma evolution during the short period between edge-localized modes (ELMs). Immediately after the ELM steep gradients in pressure, P, and density, ne, form pedestals close to the separatrix, and they then expand into the core. Local gyrokinetic analysis over the ELM cycle reveals the dominant microinstabilities at perpendicular wavelengths of the order of the ion Larmor radius. These are kinetic ballooning modes (KBMs) in the pedestal and microtearing modes (MTMs) in the core close to the pedestal top. The evolving growth rate spectra, supported by gyrokinetic analysis using artificial local equilibrium scans, suggest a new physical picture for the formation and arrest of this pedestal.Comment: Final version as it appeared in PRL (March 2012). Minor improvements include: shortened abstract, and better colour table for figures. 4 pages, 6 figure

    Preliminary results of a provenance trial of Eucalyptus camaldulensis in a dry tropical area of north Australia

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    A provenance trial of Eucalyptus camaldulensis was conducted in the Burdekin region of tropical north Queensland, Australia. Six provenances ranging from subtropical south Queensland to tropical north Queensland, each with and without mulch at planting, were assessed for their survival, height and DBH. There was a significant difference in survival, height and DBH among the provenances tested at age three years. However, the effect of mulch on these three parameters was insignificant. It appears that for the harsh environments of dry tropical north Queensland, provenances of tropical origins are more suitable than those from subtropical areas

    Suitability of Eucalyptus grandis and E. microcorys as windbreak species in tropical northern Australia

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    A study was conducted on the Atherton Tablelands of tropical north Australia to compare the suitability of Eucalyptus grandis and E. microcorys for forming windbreaks. Wind speed was measured at various distances from the leeward side of each of the E. grandis and E. microcorys windbreaks, both 13 years old and consisting of five rows of trees. The species were measured for their height, diameter at breast height (DBH), crown length (between the rows) and width (along the row), number of branches per tree, bole length (height to the lowest branch) and windbreak porosity. The E. microcorys windbreak had a uniform porosity both vertically and horizontally while the E. grandis windbreak had uneven porosity with some obvious gaps at the base (up to 8 m from the ground). E. grandis was significantly taller and longer in bole length but lower in number of branches per tree than E. microcorys at age 13 years. Wind speed was reduced more by the E. microcorys windbreak than by the E. grandis windbreak. E. microcorys appears to be a suitable species for windbreaks whereas E. grandis does not

    Windbreak benefit to potato yield in tropical north Australia

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    A study was conducted on the Atherton Tablelands of tropical north Australia to quantify the benefit of a 18-month-old windbreak to the production of potato (Solanum tuberosum L.). In the leeward side, wind velocity and potato yield were measured at various distances from the windbreak. Wind direction on the study site was also monitored. Non-linear modeling was used to describe the relationship between potato yield and distance from the windbreak. The definite integral was applied to the developed model to calculate the net increase percentage of potato yield. Wind velocity was greatly reduced by the windbreak, and potato yield was increased by 6%. It appears that fitting non-linear models is a useful method to determine an accurate net increase of crops from windbreaks
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